1. Climate case study

2. Outline The challenge The simulator The data Definitions and conventions Elicitation Expert beliefs about climate parameters Expert beliefs about model discrepancy Analysis The emulators Calibration Future CO2 scenarios MUCM short course - session 52

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4. The challenge

5. How much CO 2 can we survive? How much CO 2 can we add to the atmosphere without increasing global mean temperature more than 2°C? Several ambiguities in this question Obviously depends on time profile of CO 2 emissions And on time horizon Two degrees increase relative to what? How to define and measure global mean temperature Even if we resolve those, how would we answer the question? Need a simulator to predict the future And much more besides! MUCM short course - session 55

6. The simulator We use the C-Goldstein simulator Three coupled model components GOLDSTEIN ocean model An Energy Moisture Balance Model based on Uvic A simple sea ice model Relatively low resolution 36 x 36 x 8 ocean layers 100 time-steps per year Spin-up to year 1800AD (3792 years of spin-up) Then forced by historic CO 2 levels From ice cores to 1957 then Mauna Loa to 2008 MUCM short course - session 56

7. C-Goldstein inputs 18 inputs All with uncertain values Need to allow for uncertainty in the analysis Last input has no effect except for future projections yielding significant warming MUCM short course - session 57

8. 8 Example of C-Goldstein output: Surface air temperature in 2000 using default input values

9. The data We have historic data on global mean temperature Decadal averages for each decade from 1850 to 2009 From HadCrut3 These are to be used to calibrate the simulator Thereby hopefully to reduce prediction uncertainty Note that the HadCrut3 data are actually values of the temperature “anomaly” Which brings us to the next slide MUCM short course - session 59

10. RGMT Two issues around defining global mean temperature (GMT) 1. Attempts to measure or model it are subject to biases It is generally argued that differences in GMT are more meaningful and robust Hence our data are differences between observed GMT in a given year and the average over 1961-1990 We call this (observed) RGMT Relative GMT The output that we take from C-Goldstein for each decade is also converted to (simulated) RGMT By subtracting average simulator output for 1961-1990 MUCM short course - session 510

11. Weather versus climate 2. HadCrut3 data show substantial inter-annual variability There is weather on top of underlying climate C-Goldstein output is much smoother Just climate We assessed the inter-annual error variance by fitting a smooth cubic And looking at decadal deviations from this line True RGMT is defined as underlying climate Observed RGMT is true RGMT plus measurement and inter-annual (weather) error Simulated RGMT is true RGMT plus input error and model discrepancy MUCM short course - session 511

12. Black line and grey error bars = HadCrut3 and measurement error Green line = cubic fit Red decadal bars = measurement (orange) plus inter-annual error MUCM short course - session 512

13. Target 2 degree rise The target of keeping with 2 degrees warming was defined as Relative to pre-industrial temperature For future up to year 2200 So max true RGMT should be less than (pre-industrial + 2) The objective was to assess the probability of achieving this target For given future CO 2 emissions scenarios Averaged with respect to all sources of uncertainty After calibration to historic RGMT data Including emulation uncertainty MUCM short course - session 513

14. Elicitation

15. Parameter distributions Uncertainty about the 18 C-Goldstein inputs was characterised as probability distributions True values defined to give best fit to historic RGMT Obtained by eliciting judgements from 2 experts Using the SHELF elicitation framework http://tonyohagan.co.uk/academic/shelf E.g. Ocean Drag Coefficient Default value = 2.5 Elicited range = [0.6, 4.4] Distribution = Gamma(3.51, 1.62) MUCM short course - session 515

16. Model discrepancy Beliefs about discrepancy between C-Goldstein RGMT and true RGMT also elicited From the same two experts Defined for true values of inputs Predicting ahead to year 2200 Experts thought model discrepancy would grow with temperature The higher the temperature, the further we get from where we can check the simulator against to reality Simulator error will grow rapidly as we extrapolate Complex and difficult elicitation exercise Details in toolkit MUCM short course - session 516

17. Analysis

18. Two emulators We built two separate emulators 1. Emulation of the decadal simulated RGMT As a function of 17 inputs Multivariate GP emulator Used for calibration against the historic temperature data 2. Emulation of future max simulated RGMT Up to year 2200 As a function of 18 inputs and 3 scenario parameters Used for assessing probability of staying under 2 degrees warming MUCM short course - session 518

19. The first emulator C-Goldstein takes about one hour to spin-up and run forward to 2008 We ran it 256 times to create a training sample According to a complex design strategy – see the toolkit! After removing runs where no result or implausible results were obtained, we had 204 runs The multivariate emulator was built And validated on a further 79 (out of 100) simulator runs Validation was poor over the baseline period 1961-90 but otherwise good MUCM short course - session 519

20. 95% of these standardised errors should lie within the red lines We see problems with outputs 12 to 14 (1960s to 80s) And results rather too good at the earliest and latest dates Partly the fault of multivariate GP MUCM short course - session 520

21. Calibration After allowing for model discrepancy, the decadal data provide little information about any of the input parameters All training runs consistent with decadal data and the elicited discrepancy We do learn about the shape of the discrepancy Calibration suggests it increases even faster with temperature But this is largely coming from the final observations, and so may be unreliable MUCM short course - session 521

22. The second emulator – training runs Future scenarios for atmospheric CO 2 concentrations are governed by 3 parameters, t 1, dx and dy Each of the original spin-ups was run forward to 2200 with 64 comb- inations of these 3 parameters Black lines Validation spin-ups were run forward with 30 combinations Green lines MUCM short course - session 522

23. Computing probabilities of target The second emulator was built for the max RGMT output And validated well Particularly well when temperature rise was smaller Probability of true RGMT rise staying below a specific threshold Computed by averaging emulator predicted probabilities Averaged over the sample of calibrated parameter values Allowing for discrepancy and emulation uncertainties Calculation can be done for any (t 1, dx, dy) and any threshold We used 2, 4 and 6 degrees MUCM short course - session 523

24. Red lines are for 2 degrees warming Green for 4 degrees and blue for 6 Each frame shows probability as a function of t 1 Chance of staying under 2 degrees decreases the later we act And the faster we increase CO 2 before acting And the slower we decrease thereafter That’s as expected of course, but now we have quantitative assessments of the chance MUCM short course - session 524

25. Conclusions We can now see just how early and how hard we must act on CO 2 emissions In order to have a good chance of staying under 2 degrees Lots of caveats, of course In particular, it’s dependent on the expert elicitation of C-Goldstein model discrepancy We have very little data to check those judgements But nobody has attempted to include that factor before This is pioneering work! Emulation was crucial Even for a moderate complexity model like C-Goldstein MUCM short course - session 525